烷基取代聚噻吩的非等温结晶动力学

根据ＤＳＣ测得的数值,采用Ｊｅｚｉｏｒｎｙ ,Вороховский和由作者实验室提出的一种新方法研究了十二烷基取代聚噻吩（Ｐ３ＤＤＴ） 和十八烷基取代聚噻吩（Ｐ３ＯＤＴ） 的非等温结晶过程,并应用Ｋｉｓｓｉｎｇｅｒ 法求取其结晶表观活化能ΔＥ,探讨了不同烷基取代基团对结晶过程的影响．Ｐ３ＤＤＴ 应用Ｊｅｚｉｏｒｎｙ 和Вороховский法描述时在结晶后期均发生偏离现象,而作者提出的新方法描述时则得到较好的线性关系．求得Ｐ３ＤＤＴ 的ΔＥ 为１８４－７９ｋＪ／ｍｏｌ,Ｐ３ＯＤＴ 的ΔＥ 为２４６－９３ｋＪ／ｍｏｌ,比较结晶表观活化能数值可知,Ｐ３ＤＤＴ 比Ｐ３ＯＤＴ 更易结晶．     

O-(4-喹唑啉)羟肟酸硫代酯(酰胺)类化合物的合成及生物活性

用差示扫描量热分析研究了间规聚苯乙烯（ｓＰＳ）的非等温结晶及其动力学，并分别用Ｏｚａｗａ和Ｊｅｚｉｏｒｎｙ两种方法来处理ｓＰＳ的非等温结晶数据．结果表明，在２５～４０℃／ｍｉｎ的冷却速率范围内，ｓＰＳ的半结晶时间随冷却速率增大而呈指数式下降，ｓＰＳ非等温结晶过程遵循Ｏｚａｗａ动力学方程，但不符合Ｊｅｚｉｏｒｎｙ方法中的Ａｖｒａｍｉ动力学方程．所得到的ｓＰＳ非等温结晶Ａｖｒａｍｉ指数ｎ在３６～４１之间，高于等温结晶时的ｎ值     

在（TPA）2O—Na2O—SiO2—H2O系统中MFI型硅沸石的结晶行为（I）：结…

以四丙基溴化铵作模板剂，以白炭黑（Ｉ）、硅溶胶（Ⅱ）和水玻璃（Ⅲ）为不同硅源在１４０￣１８０℃合成ＭＦＩ型硅沸石。反应物配比相同，其结晶动力学曲线有明显差异。从它们的成核诱导期及生长速度计算出各体系硅沸石晶核形成活化能与生长活化能，在体系（Ｉ）中为４６／７６ｋＪ／ｍｏｌ，体系（Ⅱ）中为４１／４３ｋＪ／ｍｏｌ，体系（Ⅲ）中为３８／７９ｋＪ／ｍｏｌ。产物结晶粒径的大小由各体系成核活化能与生长活化能的差     

聚丙烯接枝马来酸酐及其离聚物的非等温结晶动力学

用 Ｄ Ｓ Ｃ 测定了固相接枝法制备的聚丙烯接枝马来酸酐（ Ｐ Ｐ ｇ Ｍ Ａ Ｈ） 及其３ 种５ 个离聚物在不同冷却速率的非等温结晶动力学．分析了结晶峰温（ Ｔｍａｘ） 、结晶起始温度（ Ｔ０） 、结晶峰的初始斜率（ Ｓｉ） 及结晶峰的半高宽（ Δｗ ） 等结晶峰参数;用 Ａｖｒａｍｉ 方程和综合了 Ａｖｒａｍｉ Ｏｚａｗａ 方程的方法处理非等温结晶动力学．对于全部样品在所有的冷却速率下, Ａｖｒａｍｉ 指数ｎ 值均在２５ ～２８ 之间,说明聚丙烯结晶行为没有改变;但同时发现接枝及离子化后,成核速率加快,晶粒分布变窄,结晶总速率增大,与等温结晶动力学得到的结论一致．     

聚丙烯接枝马来酸酐及其离聚物的等温结晶行为

采用ＤＳＣ对马来酸酐接枝聚丙烯（ＰＰ ｇ ＭＡＨ）及其３种５个离聚物的等温结晶行为进行了研究,发现在相对结晶度２％～９０％的范围内符合Ａｖｒａｍｉ方程．马来酸酐的引入及离子化并不改变ＰＰ的结晶行为,但样品的结晶速率增大,同时结晶速率亦随中和度的提高而增大．从Ｈｏｆｍａｎ理论得到７个样品的垂直于晶核的界面自由能σｅ,其变化与Ａｖｒａｍｉ方程的结果是一致的．     

聚苯乙炔LB多层膜及其光电导性能的研究

制备了聚苯乙炔（ＰＰＡ）ＬＢ多层膜，将其作为电荷产生层首次应用于机能分离型光电导体领域．从π Ａ曲线发现，ＰＰＡ单分子膜具有表面压力的各向异性和松弛特性．ＴＥＭ照片显示，ＰＰＡ分子链在ＬＢ膜中有序排列．转移比和ＸＰＳ的研究表明，复合膜沉积均匀．与ＰＰＡ涂膜相比，以ＰＰＡ ＬＢ多层膜作为电荷产生层的光电导体表面充电电位Ｖ０＝１３４５Ｖ，光照１ｓ后的光衰百分比ΔＶ１ｓ＝６５０５％，半衰时间ｔ１／２＝０５８ｓ，具有更优异的光电导性能．     

鸟嘌呤—铜配合物在汞电极表面上的电吸附性的研究

在０．０２ｍｏｌ／Ｌ ＮａＨＣＯ３－０．０５ｍｏｌ／Ｌａ２ＳＯ４介质中、用极谱法和伏安法研究表明,铜－乌嘌呤配合物在汞电极表面上的吸附服从Ｌａｎｇｍｕｉｒ吸附,测得其饱和吸附量Γｍ＝１．１×１０＾－１０ｍｏｌ／ｃｍ＾２,吸附系数β＝４．７×１０＾４,吸咐自由能△Ｇ°＝－３６．６ｋＪ／ｍｏｌ。在８×１０＾－６ｍｏｌ／Ｌ Ｃｕ＾２＋离子存在下,可用示差脉冲阴极吸附溶出法测定８×１０＾－１０～１×１０＾     

聚氧化乙烯梳状聚合物共混物的非等温结晶动力学

用ＤＳＣ方法对乙烯基甲醚／马来酸酐交替共聚物多缩乙二醇酯（ＣＢＰ） 聚氧化乙烯（ＰＥＯ）共混体系的非等温结晶动力学进行了研究，用Ｍａｎｄｅｌｋｅｒｎ、Ｚ Ｊ（Ｚｉａｂｉｋｉ Ｊｅｚｉｏｒｎｙ）、Ｏｚａｗａ和对Ｏｚａｗａ方法的一种修正方法对该体系进行了处理．结果表明：得到了一种既没有结晶又有较多ＥＯ单元含量的共混物，ＣＢＰ对ＰＥＯ的结晶有抑制作用．Ａｖｒａｍｉ指数随冷却速率的加快在３８～５７之间波动．Ｍａｎｄｅｌｋｅｒｎ方法求得的结晶动力学参数Ｚｃ随冷却速率的增加而增加，共混物的Ｇｃ值不随冷却速率的变化而变化，随ＰＥＯ含量增加而减少，处理结果表明而Ｚ Ｊ理论能较好地解释本体系的非等温结晶过程和机理．     

Pt／NM,Pd／NM催化剂上甲苯深度氧化反应动力学

在氧气过量的条件下，考察了Ｐｔ／ＮＭ、Ｐｄ／ＮＭ催化剂上甲苯深度氧化反应动力学及反应活性。Ｐｔ／ＮＭ催化剂对甲苯的氢化活性高于Ｐｄ／ＮＭ，深度氧化反应服从反应物强吸附双分子反应Ｌｔａｎｇｍｕｉｒ－Ｈｉｎｓｈｅｌｗｏｏｄ机理，其动力学方程为：相应的动力学参数，Ｐｔ／ＮＭ为：活化能△Ｅ＝４９．９ｋＪ／ｍｏｌ，吸附热Ｑ＝－２９．６ｋＪ／ｍｏｌ；Ｐｄ／ＮＭ为：△Ｅ＝９４．２ｋＪ／ｍｏｌ，Ｑ＝－１９．１ｋＪ／ｍｏｌ．     

金属离子与卟啉的嵌入反应动力学研究──Ⅶ．一元酸根催化Cu（Ⅱ）与溴化间－四（N－乙酸甲酯基－3－吡啶基）卟啉的配位反应

研究了在３５±０．１℃、离子强度０．５ｍｏｌ／Ｌ（ＫＣｌ）条件下，甲酸根、乙酸根、丙酸根和丁酸根分别催化Ｃｕ（Ⅱ）离子与四溴化间－四（Ｎ－乙酸甲酯基－３－吡啶基）卟啉（Ｈ２ＴＢ－Ｎ－ＡＣＭＳｐｙＰＢｒ４）的反应动力学及其机理，该类反应对卟啉和Ｃｕ（Ⅱ）离子均为一级反应，反应动力学方程为：ｄ［Ｃｕｐ４＋］／ｄｔ＝ｋ｛（１．０＋ｂ［Ａ－］）／（１．０＋Ｋ３，４·［Ｈ＋］２）｝［Ｃｕ２＋］［ｐ］Ｔ，在甲酸－甲酸根缓冲体系中，ｋ＝２．９８ｍｏｌ－１ｄｍ３·ｓｅｃ－１，ｂ＝１５４×１０２ｍｏｌ－２，ｄｍ６·ｓｅｃ－１，Ｋ３，４＝６．９２８×１０３；在乙酸－乙酸根缓冲体系中，ｋ＝３．４２ｍｏｌ－１·ｄｍ３·ｓｅｃ－１，ｂ＝２．２９×１０３ｍｏｌ－２·ｄｍ６·ｓｅｃ－１，Ｋ３，４＝６．９２８×１０３；在丙酸－丙酸根缓冲体系中，ｋ＝３．００ｍｏｌ－１·ｄｍ３·ｓｅｃ－１，ｂ＝５．９０×１０２ｍｏｌ－２·ｄｍ６·ｓｅｃ－１，Ｋ３，４＝７．００７×１０３；在丁酸－丁酸根缓冲体系中，ｋ＝３．１４ｍｏｌ－１·ｄｍ３·ｓｅｃ－１，ｂ＝３．７５×１０２ｍｏｌ－２·ｄｍ６·ｓｅｃ－１，Ｋ３，４＝６．９２１×１０３；讨论了有机酸根的碱性与     

MELTING CRYSTALLIZATION BEHAVIOR OF NYLON 66

Analysis of isothermal and nonisothermal crystallization kinetics of nylon 66 was carried out using differentialscanning calorimetry (DSC). The commonly used Avrami equation and that modified by Jeziorny were used, respectively, tofit the primary stage of isothermal and nonisothermal crystallizations of nylon 66, In the isothermal crystallization process,mechanisms of spherulitic nucleation and growth were discussed. The lateral and folding surface free energies determinedfrom the Lauritzen-Hoffman treatment are σ= 9.77 erg/cm~2 and σ_e= 155.48 erg/cm~2, respectively; and the work of chainfolding is q = 33.14 kJ/mol. The nonisothermal crystallization kinetics of nylon 66 was analyzed by using the Mo methodcombined with the Avrami and Ozawa equations. The average Avrami exponent n was determined to be 3.45, Theactivation energies (ΔE) were determined to be -485.45 kJ/mol and -331.27 kJ/mol, respectively, for the isothermal andnonisothermal crystallization processes by the Arrhenius and the Kissinger methods.     

Isothermal and nonisothermal crystallization kinetics of nylon‐46

Isothermal and nonisothermal crystallization kinetics of nylon‐46 were investigated with differential scanning calorimetry. The equilibrium melting enthalpy and the equilibrium melting temperature of nylon‐46 were determined to be 155.58 J/g and 307.10 °C, respectively. The isothermal crystallization process was described by the Avrami equation. The lateral surface free energy and the end surface free energy of nylon‐46 were calculated to be 8.28 and 138.54 erg/cm², respectively. The work of chain folding was determined to be 7.12 kcal/mol. The activation energies were determined to be 568.25 and 337.80 kJ/mol for isothermal and nonisothermal crystallization, respectively. A convenient method was applied to describe the nonisothermal crystallization kinetics of nylon‐46 by a combination of the Avrami and Ozawa equations. © 2002 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 40: 1784–1793, 2002     

Isothermal and nonisothermal crystallization kinetics of novel odd-odd polyamide 9 11

A study on isothermal and nonisothermal crystallization kinetics of odd-odd polyamide 9 11 was carried out by differential scanning calorimetry (DSC). The equilibrium melting temperature of polyamide 9 11 was determined to be 199.1 °C. The Avrami equation was adopted to describe isothermal crystallization of polyamide 9 11. Nonisothermal crystallization was analyzed using both the Avrami relation modified by Jeziorny and the equation suggested by Mo. The isothermal and nonisothermal crystallization activation energies of polyamide 9 11 were determined to be −310.9 and −269.0 kJ/mol using the Arrhenius equation and the Kissinger method, respectively.     

聚醚醚酮酮等温结晶动力学的研究

聚醚醚酮酮等温结晶动力学的研究陈艳，王军佐，曹俊奎，那辉，吴忠文（吉林大学化学系，长春，１３００２３）关键词聚醚醚酮酮，等温结晶动力学，差示扫描量热法聚醚醚酮酮（ＰＥＥＫＫ）是在聚醚醚酮（ＰＥＥＫ）基础上开发成功的一种耐热高分子材料。它保持了ＰＥＥＫ...     

Melting behaviors,crystallization kinetics,and spherulitic morphologies of poly(butylene succinate) and its copolyester modified with rosin maleopimaric acid anhydride

This article investigated the melting behaviors, crystallization kinetics, and spherulitic morphologies of poly(butylene succinate) (PBS) and its copolyester (PBSR) modified with rosin maleopimaric acid anhydride, using wide‐angle X‐ray diffraction, differential scanning calorimeter (DSC), and polarized optical microscope. Subsequent DSC scans of isothermally crystallized PBS and PBSR exhibited two melting endotherms, respectively, which was due to the melt‐recrystallization process occurring during the DSC scans. The equilibrium melting point of PBSR (125.9 °C) was lower than that of PBS (139 °C). The commonly used Avrami equation was used to describe the isothermal crystallization kinetics. For nonisothermal crystallization studies, the model combining Avrami equation and Ozawa equation was employed. The result showed a consistent trend in the crystallization process. The crystallization rate was decreased, the perfection of crystals was decreased, the recrystallization was reduced, and the spherulitic morphologies were changed when the huge hydrogenated phenanthrene ring was added into the chain of PBS. The activation energy (ΔE) for the isothermal crystallization process determined by Arrhenius method was 255.9 kJ/mol for PBS and 345.7 kJ/mol for PBSR. © 2006 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 44: 900–913, 2006     

Isothermal and nonisothermal crystallization kinetics of irradiated nylon 1212

The crystallization behavior of nylon 1212, irradiated at ⁶⁰Co γ‐rays (50 kGy), was studied by a rheometer, polarized optical microscopy (POM), and differential scanning calorimeter (DSC). The results showed that irradiated nylon 1212 samples exhibited abnormal crystallization behavior during the crystallization process: The Avrami exponent n was calculated and was found to be in the range from 2.06–2.41 for isothermal crystallization, and from 2.67–4.91 for nonisothermal crystallization; the spherulite morphology also changed largely by polarized optical microscopy (POM); the crystallization activation energy ΔE for isothermal and nonisothermal crystallization process of irradiated nylon 1212 are determined to be 57.4 kJ/mol and 78.65 kJ/mol, respectively, which are lower than that of nonirradiated nylon 1212. At the same time, a new method by a combination of the Avrami and Ozawa equations was successfully applied to analyze the noncrystallization process of irradiated nylon 1212. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 2326–2333, 2005     

Morphology, isothermal and non-isothermal crystallization kinetics of poly(methylene terephthalate)

The morphology of crystals, isothermal and non-isothermal crystallization of poly(methylene terephthalate) (PMT) have been investigated by using polarized optical microscopy and differential scanning calorimeter (DSC). The POM photographs displayed only several Maltese cross at the beginning short time of crystallization indicating that some spherulites had been formed. The crystal cell belonged to the Triclinic crystal systems and the cell dimensions were calculated from the WAXD pattern. The commonly used Avrami equation and that modified by Jeziorny were used, respectively, to fit the primary stage of isothermal and non-isothermal crystallization. The Ozawa theory was also used to analyze the primary stage of non-isothermal crystallization. The Avrami exponents n were evaluated to be in the range of 2-3 for isothermal crystallization, and 3-4 for non-isothermal crystallization. The Ozawa exponents m were evaluated to be in the range of 1-3 for non-isothermal crystallization in the range of 135-155 °C. The crystallization activation energy was calculated to be −78.8 kJ/mol and −94.5 kJ/mol, respectively, for the isothermal and non-isothermal crystallization processes by the Arrhenius’ formula and the Kissinger’s methods.     

不同分子量聚L-乳酸的非等温结晶动力学研究

采用DSC方法研究了不同分子量聚乳酸在不同降温速率下的结晶过程,利用Ozawa方程和Kissinger方程研究了其非等温结晶动力学。结果表明,随着降温速率的增大和分子量增加,结晶峰向低温偏移,且峰形趋于平缓。求得分子量为2.6×104的聚乳酸的Ozawa指数m接近3,以异相成核的三维球晶生长为主,而分子量为14.3×104和19.2×104的聚乳酸的Ozawa指数m接近4,以均相成核的三维球晶生长为主,结晶活化能分别为-165.8kJ/mol、-82.1kJ/mol和-75.4kJ/mol。建立的"铰链"模型解释了不同分子量聚乳酸结晶活化能的显著差异,得到了聚乳酸分子量与结晶活化能的关系。     

窄分子量分布茂金属短链支化聚乙烯结晶动力学

本工作用DSC方法对三种不同支化度的茂金属短链支化聚乙烯的等温、非等温结晶行为进行了研究 .样品为乙烯和己烯 1的共聚物 ,短支链主要为正丁基 ,分子量Mw =2 0 ,0 0 0 ,Mw/Mn<1 15 ,支化度 (每10 0 0C中CH3 数目 )分别为 1 6、10 4、40 .实验结果表明 ,茂金属短链支化聚乙烯结晶方式Ⅰ Ⅱ转变温度随支化度增加而降低 ,分别为 119 8℃、115 9℃、113 3℃ ;同时支链的存在降低了二次成核速率 ,增大了方式Ⅰ的结晶范围 ,总的结晶速度随支化度增大而减小